Article ID Journal Published Year Pages File Type
1646478 Materials Letters 2012 4 Pages PDF
Abstract

The band alignment and the quantum states of InAsxP1−x/InP surface quantum well (SQW) are investigated using ultraviolet photoelectron spectroscopy (UPS) and photoluminescence techniques. The analysis of UPS spectra of core levels In 4d, As 3d, P 3p and P 2p confirms that the top surface of InAsxP1−x/InP SQW contains an admixture of oxides, which convert into a more stable form of oxide, In(PO3)3, after optimum Ar+ ion sputtering. The values of valence band offsets between In(PO3)3/InP and InAsxP1−x/InP (x=0.57) SQW are 2.1 eV and 0.3 eV respectively, as obtained from the onsets of UPS spectra. Further, the band structure of InAsxP1−x/InP SQW is also estimated from the UPS spectra of core levels and the valence band onsets after optimum Ar+ ion sputtering. The emission of the quantum states (e1–hh1) transition blue-shifts by about 60 meV for InAs0.38P0.62/InP SQW when the top InP barrier layer thickness is decreased from 22 Å to 11 Å. The experimental values of e1–hh1 electronic transition in SQW match well with those of the theoretically calculated ones using a 3.6 eV potential barrier at the InP surface.

► Top surface of InAsxP1−x/InP SQW contains an admixture of oxides, which convert into the more stable In(PO3)3 after Ar+ ion sputtering. ► Values of valence band offsets between In(PO3)3/InP and InAsxP1−x/InP (x=0.57) SQW are 2.1 eV and 0.3 eV respectively. ► Band structure of InAsxP1−x/InP SQW estimated from the UPS spectra of core levels and the valence band onsets after optimum Ar+ ion sputtering. ► Emission of quantum states (e1–hh1) transition blue-shifts by about 60 meV for InAs0.38P0.62/InP SQW when the top InP barrier layer thickness is decreased from 22 Å to 11 Å. ► Experimental values of e1–hh1 electronic transition in SQW match well with those of the theoretically calculated ones using a 3.6 eV potential barrier at the InP surface.

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Physical Sciences and Engineering Materials Science Nanotechnology
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